CN103064071A - Radar target attribute scattering center feature extraction method based on sparse decomposition - Google Patents

Radar target attribute scattering center feature extraction method based on sparse decomposition Download PDF

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CN103064071A
CN103064071A CN201210414929XA CN201210414929A CN103064071A CN 103064071 A CN103064071 A CN 103064071A CN 201210414929X A CN201210414929X A CN 201210414929XA CN 201210414929 A CN201210414929 A CN 201210414929A CN 103064071 A CN103064071 A CN 103064071A
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scattering center
parameter
dictionary
scattering
vector
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CN103064071B (en
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刘宏伟
李飞
纠博
杜兰
王英华
王鹏辉
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Xidian University
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Abstract

The invention discloses a radar target attribute scattering center feature extraction method based on sparse decomposition. The radar target attribute scattering center feature extraction method based on the sparse decomposition mainly solves the problems in an existing method capable of segmenting an image to extract attribute scattering center based on the radar image that models are unmatched, features are easy to lose, and parameter estimation accuracy is low. The implementation process includes the following steps: building a scattering center intensity threshold by using noise samples, conducting an intensive scattering center test in the radar image and confirming a values set of a scattering center parameter, obtaining a target attribute scattering center parameter super-resolution estimation set according to attribute scattering center models by using coordinate repeated decline technology to build a super-resolution dictionary through solving the problem of 0 norm optimization, and extracting geometric dimensioning features of the target and important components of the target according to the scattering center parameter set. The radar target attribute scattering center feature extraction method based on the sparse decomposition is capable of effectively extracting the target attribute scattering center and the super-resolution scattering center parameter, accurately estimating the geometric dimensioning features of the target and the important components of the target, and can be used for radar target classification and identification.

Description

Radar target attribute scattering center feature extracting method based on Its Sparse Decomposition
Technical field
The invention belongs to the Radar Technology field, relate to a kind of radar target attribute scattering center feature extracting method, can be used for the physical dimension of estimating target and vitals thereof, for target classification identification provides important characteristic information.
Background technology
The radar imagery technology is to grow up the 1950's, and radar image is the two-dimensional scattering figure of target.The tradition radar imagery is take the point scattering model as the basis, and this model only comprises the target scattering dot position information, but only utilize the recognition feature of the positional information structure of target scattering point can not complete sign radar image in the essential attribute of target.In optical zone, the high-frequency electromagnetic scattering response of expansion target can be with the scatterer of one group of independent distribution, or the electromagnetic scattering response sum approximate representation of title scattering center.The scattering center of target mainly results from the point of discontinuity positions such as edge, flex point, corner angle and tip of target, represented the meticulous physical arrangement of target, so scattering center model can more relevantly be described objective attribute target attribute, also in the radar target recognition field important application is arranged.
Based on geometric theory of diffraction and physical optics theory, Michael J.Gerry in 1999 and Lee C.Potter have proposed the parameterized model that is applicable to synthetic-aperture radar (SAR)-attribute scattering center model, see [M.J.Gerry, L.C.Potter, I.J.Gupta, and A.van der Merwe, A parametric model for syntheticaperture radar measurements[J] .IEEE Transactions on Antennas and Propagation, 1999, Vol.47, NO.7, pp.1179-1188].The attribute scattering center model is with position, shape, direction and the amplitude etc. of one group of each scattering center of parametric description, and these attributes all are the important informations that concerns target; Compare with the point scattering model, the attribute scattering center model has comprised the abundanter feature that can be used for target classification identification.
The feature extraction of target scattering center is a process of estimating each scattering center parameter from the target echo data in essence.Because attribute scattering center model complex structure and parameter dimension are higher, increased the complicacy of model parameter estimation.Existing method obtains the lower target scattering district of exponent number or isolated scattering center by the radar image that obtains as the basis take the point scattering model is carried out image segmentation, utilizes the attribute scattering center parameter of approximate maximum likelihood method estimating target.At first because existing method utilization is extracted the attribute scattering center according to the radar image that the point scattering model obtains, so there is the model mismatch problem; Secondly since these class methods take image segmentation as the basis, so these class methods require picture quality higher, when some parts scattering strength of target is weak, be difficult to correct the detection by image partition method in addition, this just causes some key characters of target easily to be lost.Optimization problem owing to these class methods is non-protruding problem in addition, and has a lot of local minimal solutions, thus the problem that exists parameter initialization, model order selection and scattering center structured sort to differentiate, so that the final argument estimated accuracy is lower.
Summary of the invention
The object of the invention is to propose a kind of method of the radar target attribute scattering center feature extraction based on Its Sparse Decomposition, the model mismatch, the feature that exist in the existing method are easily lost and the low problem of Parameter Estimation Precision to solve.
The present invention is achieved in that
One. technical thought
In the radar return, target scattering field overwhelming majority energy illustrates that only by the contribution of a small amount of strong scattering center radar return has very strong sparse property at the parameter space of attribute scattering center.Consider that attribute scattering center parameter space dimension is higher, the redundant dictionary dimension that causes constructing is far longer than our accessible dimension, method of the present invention is based on sparse resolution theory, and utilize coordinate samsara decline Techniques For Reducing problem dimension and make up the super-resolution dictionary, extract attribute scattering center feature by finding the solution 0 norm optimization problem; Set up the scattering center strength threshold and in radar image, carry out the strong scattering Spot detection, determine the value set of scattering center parameter in conjunction with prior imformation; According to the attribute scattering center model, utilize coordinate samsara descent method technique construction super-resolution dictionary, obtain the parameter estimation set of attribute scattering center and target and vitals geometries characteristic thereof.
Two. technical scheme
Performing step of the present invention comprises as follows:
1) sets scattering center strength threshold ξ according to noise in the radar image, intensity in the radar image is defined as the strong scattering center greater than the scattering center of ξ, according to the strong scattering centre coordinate (x that detects, y) determine coordinate parameters x, the span of y, determine scattering center length L span by prior imformation, set distributed scattering center position angle
Figure BDA00002308719300021
Final definite scattering center parameter Set
Figure BDA00002308719300023
2) according to described parameter sets
Figure BDA00002308719300024
Make up dictionary
Figure BDA00002308719300025
2a) with dictionary
Figure BDA00002308719300026
Parameter sets
Figure BDA00002308719300027
Discretize, the interval that is about to the adjacent coordinates parameter x is made as a Range resolution element length ρ r, the interval of adjacent coordinates parameter y is made as an azimuth discrimination element length ρ a, the interval of adjacent scattering center length parameter L is made as ρ a
2b) according to the attribute scattering center model, produce the atom d of corresponding different parameters i(f, φ)
d i ( f , φ ) = exp ( - j 4 πf c ( x i cos φ + y i sin φ ) ) ·
sin c ( 2 &pi;f c L i sin ( &phi; - &phi; i &OverBar; ) ) - - - < 1 >
i=1,…N 0
Wherein i represents atom sequence number, N 0Expression is dictionary when (x, y, L) according to a preliminary estimate
Figure BDA00002308719300033
The atom number, exp () is natural exponential function, sinc () is Sinc function,
Figure BDA00002308719300034
Be set
Figure BDA00002308719300035
I group parameter after the discretize, f is the radar emission signal frequency, and φ is the radar beam position angle, and c is the light velocity;
To not homoatomic d i(f, φ) column vector, and former subvector carried out energy normalized, make up dictionary For:
D 0 ( x , y , L | &theta; ^ 0 ) = [ d ^ 1 , . . . , d ^ i , . . . , d ^ N 0 ]
d ^ i = vec ( d i ( f , &phi; ) ) | | vec ( d i ( f , &phi; ) ) | | 2 - - - < 2 >
Wherein vec () expression column vector operation, || || 2Be 2 norm operators;
3) utilize orthogonal matching pursuit OMP method to find the solution suc as formula<3〉0 norm optimization problem, by σ 1Upgrade the scattering center parameter sets
Figure BDA00002308719300039
Figure BDA000023087193000310
According to a preliminary estimate set for scattering center parameter (x, y, L);
&sigma; 1 = arg min &sigma; | | &sigma; | | 0 , s . t . | | s - D 0 ( x , y , L | &theta; ^ 0 ) &CenterDot; &sigma; | | 2 &le; &epsiv; - - - < 3 >
Wherein, σ is scattering coefficient vector to be optimized, σ 1Be the scattering coefficient vector of optimizing, s is the vectorization of frequency domain observation signal matrix column, || || 0Be 0 norm operator, ε is the energy error constraint factor, and the energy Ratios that accounts for the view picture radar image according to the object support district is determined;
4) according to described parameter sets
Figure BDA000023087193000313
Make up dictionary
Figure BDA000023087193000314
4a) determine scattering center length L span according to prior imformation, the interval of adjacent scattering center length parameter L is made as ρ a, obtain dictionary The discrete value of scattering center length parameter L; Determine distributed scattering center position angle according to the orientation angular domain of radar return data recording
Figure BDA000023087193000316
Span is with adjacent distributions formula scattering center position angle parameter
Figure BDA000023087193000317
The interval be made as
Figure BDA000023087193000318
Obtain dictionary
Figure BDA000023087193000319
Distributed scattering center position angle parameter
Figure BDA00002308719300041
Discrete value; The scattering center coordinate parameters
Figure BDA00002308719300042
4b) according to scattering center length parameter L and the distributed scattering center position angle of discretize
Figure BDA00002308719300043
By formula<1〉produce former subvector, and atom is carried out energy normalized, make up dictionary
Figure BDA00002308719300044
For:
D 1 ( L , &phi; &OverBar; | &theta; ^ 1 ) = [ d ^ 1 , . . . , d ^ i , . . . , d ^ N 1 ] - - - < 4 >
N wherein 1The expression estimated parameter
Figure BDA00002308719300046
The time dictionary
Figure BDA00002308719300047
The atom number;
5) utilize orthogonal matching pursuit OMP method to find the solution suc as formula<5〉0 norm optimization problem, by σ 2Upgrade the scattering center parameter sets
Figure BDA00002308719300048
Figure BDA00002308719300049
Be parameter
Figure BDA000023087193000410
Valuation set;
&sigma; 2 = arg min &sigma; | | &sigma; | | 0 , s . t . | | s - D 1 ( L , &phi; &OverBar; | &theta; ^ 1 ) &CenterDot; &sigma; | | 2 &le; &epsiv; - - - < 5 >
σ wherein 2Be the scattering coefficient vector of optimizing;
6) according to described parameter sets
Figure BDA000023087193000413
Make up the super-resolution dictionary
Figure BDA000023087193000414
6a) with In coordinate parameters x centered by, length is ρ rNeighborhood in value, the interval of adjacent parameter x is made as ρ r/ N s, obtain dictionary
Figure BDA000023087193000416
The discrete value of coordinate parameters x, N sBe super-resolution multiple, General N s=2,4,8 ...; With
Figure BDA000023087193000417
In y centered by, length is ρ aNeighborhood in value, the interval of adjacent parameter y is made as ρ a/ N s, obtain dictionary
Figure BDA000023087193000418
The discrete value of coordinate parameters y; With
Figure BDA000023087193000419
In L centered by, length is ρ aNeighborhood in value, the interval of adjacent parameter L is made as ρ a/ N s, obtain dictionary
Figure BDA000023087193000420
The discrete value of scattering center length parameter L; Distributed scattering center position angle parameter
Figure BDA000023087193000421
6b) according to the dictionary parameter x of discretize, y, L is by formula<1〉produce former subvector, and atom is carried out energy normalized, make up the super-resolution dictionary
Figure BDA000023087193000422
D 2 ( x , y , L | &theta; ^ 2 ) = [ d ^ 1 , . . . , d ^ i , . . . , d ^ N 2 ] - - - < 6 >
Wherein, N 2Expression super-resolution dictionary
Figure BDA000023087193000424
The atom number;
7) utilize orthogonal matching pursuit OMP method to find the solution suc as formula<7〉0 norm optimization problem, by σ 3Upgrade the scattering center parameter sets The super-resolution that obtains (x, y, L) is estimated set
Figure BDA000023087193000426
With target and vitals geometries characteristic thereof;
&sigma; 3 = arg min &sigma; | | &sigma; | | 0 , s . t . | | s - D 2 ( x , y , L | &theta; ^ 2 ) &CenterDot; &sigma; | | 2 &le; &epsiv; - - - < 7 >
σ wherein 3Be the scattering coefficient vector of optimizing.
The present invention compared with prior art has the following advantages:
(1) there is the model mismatch problem in the existing method of extracting attribute scattering center feature, and because image segmentation can cause some important scattering centers of target to be easy to lose.The present invention propose based on the radar target attribute scattering center feature extracting method of Its Sparse Decomposition from the frequency domain observation data, obtain the rarefaction representation of frequency domain observation data by finding the solution 0 norm optimization problem, can effectively extract target scattering center.
(2) existing method is carried out parameter initialization and model order and is selected based on the result that radar image is cut apart, and estimates the parameter of the attribute scattering center in the radar image subregion by approximate maximum likelihood method, and the parameters precision that these class methods are estimated is lower.The inventive method is carried out Its Sparse Decomposition by utilizing coordinate samsara decline technique construction super-resolution dictionary to the frequency domain observation data, and the super-resolution that obtains radar target attribute scattering center parameter is estimated.
(3) the present invention can effectively extract target scattering center owing to the inventive method, and obtain the super-resolution estimation of scattering center parameter, so according to the scattering center parameter sets of extracting, can obtain the precise geometrical size characteristic of target and vitals thereof.
Description of drawings
Fig. 1 is process flow diagram of the present invention;
To be attribute scattering center model medium frequency dependent factor α=1 change waveform with the frequency of distance numeric field data of frequency dependent factor-alpha=0 o'clock to Fig. 2;
Fig. 3 is orientation dependent factor γ=10 in the attribute scattering center model -11Change waveform with the orientation frequency domain data of orientation dependent factor γ=0 o'clock;
Fig. 4 is the original radar image of radar target T72 tank;
Fig. 5 is by the radar image of the inventive method to the radar target T72 tank of Fig. 4 reconstruct;
Fig. 6 is original radar target D7 forklift radar image;
Fig. 7 is by the radar target D7 forklift radar image of the inventive method to Fig. 6 reconstruct.
Embodiment
One, know-why
The tradition radar image obtains as the basis take the point scattering model, and this model only comprises the target scattering dot position information, but only utilize the recognition feature of the positional information structure of target scattering point can not complete sign radar image in the essential attribute of target.In optical zone, the high-frequency electromagnetic scattering response of expansion target can be with the scatterer of one group of independent distribution, or the electromagnetic scattering response sum approximate representation of title scattering center.The attribute scattering center model is with position, shape, direction and the amplitude etc. of one group of each scattering center of parametric description, and these attributes all are the important informations that concerns target; Compare with the point scattering model, the attribute scattering center model has comprised the abundanter feature that can be used for target classification identification.
According to the attribute scattering center model as can be known, i scattering center frequency-orientation two dimension echoed signal is in the target:
E i ( f , &phi; ; &theta; i ) = A i &CenterDot; ( j f f c ) &alpha; i exp ( - j 4 &pi;f c ( x i cos &phi; + y i sin &phi; ) ) &CenterDot; - - - < 8 >
sin c ( 2 &pi;f c L i sin ( &phi; - &theta; i &OverBar; ) ) exp ( - 2 &pi;f &gamma; i sin &phi; )
Wherein, i represents the scattering center sequence number, and f is the radar emission signal frequency, and φ is the radar bearing angle, and exp () is natural exponential function, and sin c () is Sinc function, and c is the light velocity, θ iThe parameter vector that represents i scattering center
Figure BDA00002308719300063
Ai is the scattering strength of scattering center, x iBe distance dimension coordinate, y iBe azimuth dimension coordinate, L iBe the length of distributed scattering center azimuth dimension,
Figure BDA00002308719300064
Be the position angle of distributed scattering center, α iBe the frequency dependent factor, general α i∈ 1 ,-0.5,0,0.5,1}, γ iOrientation dependent factor for local formula scattering center.
By the echoed signal sum of each scattering center, can consist of target frequency-orientation two dimension echoed signal:
E ( f , &phi; ; &theta; ) = &Sigma; i = 1 M E i ( f , &phi; ; &theta; i ) , &theta; T = [ &theta; 1 T , . . . , &theta; i , . . . , &theta; M T ] - - - < 9 >
Wherein i represents scattering center sequence number, E i(f, φ; θ i) be the echoed signal of i scattering center, M is the scattering center number, θ represents M scattering center parameter matrix, () TThe expression matrix transpose operation;
With formula<9〉target echo signal express with matrix form, its expression formula is:
s=D(θ)σ+n <10>
Wherein s is target echo signal E (f, φ; Column vector θ), D (θ) is dictionary corresponding to scattering center parameter matrix θ, and σ is the scattering coefficient vector, and n represents white Gaussian noise.
In radar return, because most energy of target scattering field are only by the contribution of a small amount of strong scattering center, therefore the explanation radar return has very strong sparse property at the parameter space of attribute scattering center.According to the sparse property of radar return at the parameter space of attribute scattering center, can obtain the rarefaction representation of observation data s by finding the solution 0 norm optimization problem, and scattering center parameter estimation set, can estimating target and the geometries characteristic of vitals by the scattering center parameter sets.
Because attribute scattering center parameter space dimension is higher, the redundant dictionary dimension that causes constructing is far longer than need dimension to be processed, therefore can be by the impact on echoed signal of the frequency dependent factor-alpha in the analytic attribute scattering center model, orientation dependent factor γ, the attribute scattering center model is simplified, reduced the parameter space dimension.
Centre frequency f when radar c=9.6GHz, bandwidth B=591MHz, other scattering center parameter is 0 o'clock, only change frequency dependent factor-alpha or orientation dependent factor γ, and frequency dependent factor-alpha and orientation dependent factor γ has following impact to the frequency domain echo data:
A) because the radar relative bandwidth is less, the frequency dependent factor-alpha makes the scattering strength of scattering center in the frequency of distance dimension subtle change can occur, as shown in Figure 2, Fig. 2 (a) medium frequency dependent factor α=1 wherein, Fig. 2 (b) medium frequency dependent factor α=0.
B) because radar bearing angle φ variation range is less, the variation of local formula scattering center orientation dependent factor γ can make the scattering strength of local formula scattering center slightly change on the orientation frequency, as shown in Figure 3, orientation dependent factor γ=10 among Fig. 3 (a) wherein -11, orientation dependent factor γ among Fig. 3 (b)=0.
By above analysis as can be known, frequency dependent factor-alpha and orientation dependent factor γ are very little to target frequency domain echo data influence, so estimated parameter The time can ignore frequency dependent factor-alpha and orientation dependent factor γ, namely think frequency dependent factor-alpha=0, orientation dependent factor γ=0, then primitive attribute scattering center model formula<8〉can be reduced to:
E ^ i ( f , &phi; ; &theta; i ) = A i &CenterDot; exp ( - j 4 &pi;f c ( x i cos &phi; + y i sin &phi; ) ) &CenterDot; < 11 >
sin c ( 2 &pi;f c L i sin ( &phi; - &theta; i &OverBar; ) )
According to the attribute scattering center model after simplifying, based on Its Sparse Decomposition, utilize coordinate samsara decline technology, the super-resolution that can obtain the target scattering center parameter estimates, can estimating target and the geometries characteristic of vitals by the scattering center parameter sets.
Two, performing step
With reference to Fig. 1, performing step of the present invention is as follows:
Step 1 is set up scattering center strength threshold ξ and is carried out the strong scattering Spot detection, determines scattering center parameter value scope.
1a) radar imagery:
By formula<11〉as can be known, radar echo signal is uniform sampling under frequency-orientation polar coordinate space, and radar imagery resamples echoed signal or interpolation, obtains at cartesian coordinate system (f x, f y) the echoed signal E (f of lower uniform sampling x, f y), f wherein xBe frequency of distance, f yBe the orientation frequency;
f x=fcos(φ),f y=fsin(φ) <12>
Wherein, φ is the radar bearing angle;
To echoed signal E (f x, f y) do two-dimentional inverse Fourier transform, obtain the radar image of target;
1b) strong scattering Spot detection, determine scattering center parameter value scope:
Set scattering center strength threshold ξ according to noise in the radar image, intensity in the radar image is defined as the strong scattering center greater than the scattering center of ξ, according to the strong scattering centre coordinate (x that detects, y) determine coordinate parameters x, the span of y, determine scattering center length L span by prior imformation, set distributed scattering center position angle Final definite scattering center parameter
Figure BDA00002308719300082
Set
Figure BDA00002308719300083
For example, when radar image data for open MSTAR measured data in the position angle be that 80.774185 ° of angles of pitch are when being 15 ° T72 tank data, set scattering center strength threshold ξ=0.28 according to noise in the radar image, the span of the scattering center range coordinate parameter x of determining is [11.1675,14.467] rice, and the span of azimuthal coordinates parameter y is [13.40625,4.875] rice, scattering center length L span is [0,4.0625] rice, distributed scattering center position angle
Figure BDA00002308719300084
Step 2 is according to described parameter sets
Figure BDA00002308719300085
Make up dictionary
Figure BDA00002308719300086
2a) with dictionary
Figure BDA00002308719300087
Parameter sets
Figure BDA00002308719300088
Discretize, the interval that is about to the adjacent coordinates parameter x is made as a Range resolution element length ρ r, the interval of adjacent coordinates parameter y is made as an azimuth discrimination element length ρ a, the interval of adjacent scattering center length parameter L is made as ρ a
For example, when radar image data for open MSTAR measured data in the position angle be that 80.774185 ° of angles of pitch are when being 15 ° T72 tank data, set scattering center strength threshold ξ=0.28 according to noise in the radar image, the span of the scattering center range coordinate parameter x of determining is [11.1675,14.467] rice, the adjacent coordinates parameter x is spaced apart 0.2538 meter, the span of azimuthal coordinates parameter y is [13.40625,4.875] rice, the interval of adjacent coordinates parameter y is made as 0.203125 meter, scattering center length L span is [0,4.0625] rice, the interval of adjacent scattering center length parameter L is made as 0.203125 meter, distributed scattering center position angle
Figure BDA00002308719300091
2b) according to the attribute scattering center model, produce the atom d of corresponding different parameters i(f, φ):
d i ( f , &phi; ) = exp ( - j 4 &pi;f c ( x i cos &phi; + y i sin &phi; ) ) &CenterDot;
sin c ( 2 &pi;f c L i sin ( &phi; - &phi; i &OverBar; ) ) - - - < 13 >
i=1,…N 0
Wherein, f is the radar emission signal frequency, and φ is the radar bearing angle, and exp () is natural exponential function, and sin c () is Sinc function, and c is the light velocity, and i represents atom sequence number, N 0Expression is dictionary when (x, y, L) according to a preliminary estimate
Figure BDA00002308719300094
The atom number, Be set
Figure BDA00002308719300096
I group parameter after the discretize.
2c) incite somebody to action not homoatomic d i(f, φ) column vector, and former subvector carried out energy normalized, make up dictionary
Figure BDA00002308719300097
D 0 ( x , y , L | &theta; ^ 0 ) = [ d ^ 1 , . . . , d ^ i , . . . , d ^ N 0 ]
d ^ i = vec ( d i ( f , &phi; ) ) | | vec ( d i ( f , &phi; ) ) | | 2 <14>
i=1,…N 0
Wherein, i represents atom sequence number, N 0Expression is dictionary when (x, y, L) according to a preliminary estimate
Figure BDA000023087193000910
The atom number, the operation of vec () expression column vector, || || 2Be 2 norm operators.
Step 3 utilizes orthogonal matching pursuit OMP to find the solution suc as formula<15〉0 norm optimization problem:
&sigma; 1 = arg min &sigma; | | &sigma; | | 0 , s . t . | | s - D 0 ( x , y , L | &theta; ^ 0 ) &CenterDot; &sigma; | | 2 &le; &epsiv; - - - < 15 >
Wherein σ is scattering coefficient vector to be optimized, σ 1Be the scattering coefficient vector of optimizing, s is the vectorization of frequency domain observation signal matrix column, || || 0Be 0 norm operator, ε is the energy error constraint factor, and it is determined according to the energy Ratios that the object support district accounts for the view picture radar image.
The solution procedure of this step is as follows:
3a) input dictionary
Figure BDA00002308719300101
3b) initialization is about to signal margin r and is initialized as frequency domain observation signal matrix column vector s, and scattering coefficient vector σ is initialized as 0, and atom index vector a is initialized as sky, establishes primary iteration number of times k=1, and the beginning iteration;
3c) the related coefficient of Dictionary of Computing and signal margin r vector C
C = D 0 ( x , y , L | &theta; ^ 0 ) H &CenterDot; r - - - < 16 >
Wherein () HThe expression conjugate transpose, the sequence number of greatest member is a among the related coefficient vector C k, can get atom index vector a and be:
a=[a 1,…,a k] <17>
3d) utilize least square method calculation method for scattering coefficient vector σ
Figure BDA00002308719300103
Wherein
Figure BDA00002308719300104
The expression pseudoinverse, D 0(:, a) be dictionary D 0Middle row number are a iThe matrix i=1 that consists of of k column vector ..., k, k are the current iteration number of times;
Upgrade surplus r:
r=s-D 0(:,a)·σ(a) <19>
Wherein σ (a) is a for sequence number among the scattering coefficient vector σ iThe column vector i=1 that consists of of k element ..., k;
3e) calculate reconstruct energy Ratios η k
&eta; k = &Sigma; | | s k | | 2 2 &Sigma; | | s | | 2 2 - - - < 20 >
s k=D 0(:,a)·σ(a)
S wherein kBe reconstruction signal, Represent 2 norms square;
If 3f) η kK-1≤ δ stops iteration, σ 1=σ, wherein δ is the thresholding of the difference of adjacent iteration energy Ratios, gets δ=0.001; Otherwise k=k+1 also goes to step 3c).
Step 4 is by the scattering coefficient vector σ that optimizes 1Upgrade the scattering center parameter sets
Figure BDA00002308719300108
According to a preliminary estimate set for scattering center parameter (x, y, L).
Step 5 is according to described parameter sets
Figure BDA00002308719300111
Make up dictionary
Figure BDA00002308719300112
5a) determine scattering center length L span according to prior imformation, the interval of adjacent scattering center length parameter L is made as ρ a, obtain dictionary The discrete value of scattering center length parameter L; Determine distributed scattering center position angle according to the orientation angular domain of radar return data recording
Figure BDA00002308719300114
Span is with adjacent distributions formula scattering center position angle parameter
Figure BDA00002308719300115
The interval be made as
Figure BDA00002308719300116
Obtain dictionary
Figure BDA00002308719300117
Distributed scattering center position angle parameter Discrete value; The scattering center coordinate parameters
Figure BDA00002308719300119
For example, when radar image data for open MSTAR measured data in the position angle be that 80.774185 ° of angles of pitch are when being 15 ° T72 tank data, scattering center length L span is [0,4.0625] rice, the interval of adjacent scattering center length parameter L is made as 0.203125 meter, distributed scattering center position angle
Figure BDA000023087193001110
Span be [3 °, 3 °], with adjacent distributions formula scattering center position angle parameter
Figure BDA000023087193001111
The interval be made as 0.25 °.
5b) according to scattering center length parameter L and the distributed scattering center position angle of discretize
Figure BDA000023087193001112
By formula<13〉produce former subvector, and former subvector is carried out energy normalized, make up dictionary
Figure BDA000023087193001113
For:
D 1 ( L , &phi; &OverBar; | &theta; ^ 1 ) = [ d ^ 1 , . . . , d ^ i , . . . , d ^ N 1 ] - - - < 21 >
Wherein, i represents the atom sequence number, i=1 ... N 1, N 1The expression estimated parameter
Figure BDA000023087193001115
The time dictionary
Figure BDA000023087193001116
The atom number.
Step 6 utilizes orthogonal matching pursuit OMP to find the solution suc as formula<22〉0 norm optimization problem:
&sigma; 2 = arg min &sigma; | | &sigma; | | 0 , s . t . | | s - D 1 ( L , &phi; &OverBar; | &theta; ^ 1 ) &CenterDot; &sigma; | | 2 &le; &epsiv; - - - < 22 >
σ wherein 2Be the scattering coefficient vector of optimizing, its solution procedure is as follows:
6a) input dictionary
6b) initialization is about to signal margin r and is initialized as frequency domain observation signal matrix column vector s, and scattering coefficient vector σ is initialized as 0, and atom index vector a is initialized as sky, establishes primary iteration number of times k=1, and the beginning iteration;
6c) the related coefficient of Dictionary of Computing and signal margin r vector C
C = D 1 ( L , &phi; &OverBar; | &theta; ^ 1 ) H &CenterDot; r - - - < 23 >
Wherein () HThe expression conjugate transpose, the sequence number of greatest member is a among the related coefficient vector C k, can get atom index vector a and be:
a=[a 1,…,a k] <24>
6d) utilize least square method calculation method for scattering coefficient vector σ
Figure BDA00002308719300122
Wherein
Figure BDA00002308719300123
The expression pseudoinverse, D 1(:, a) be dictionary D 1Middle row number are a iThe matrix i=1 that consists of of k column vector ..., k, k are the current iteration number of times;
Upgrade surplus r:
r=s-D 1(:,a)·σ(a) <26>
Wherein σ (a) is a for sequence number among the scattering coefficient vector σ iThe column vector i=1 that consists of of k element ..., k;
6e) calculate reconstruct energy Ratios η k
&eta; k = &Sigma; | | s k | | 2 2 &Sigma; | | s | | 2 2 - - - < 27 >
s k=D 1(:,a)·σ(a)
S wherein kBe reconstruction signal,
Figure BDA00002308719300125
Represent 2 norms square;
If 6f) η kK-1≤ δ stops iteration, σ 2=σ, wherein δ is the thresholding of the difference of adjacent iteration energy Ratios, gets δ=0.001; Otherwise k=k+1 also goes to step 6c).
Step 7 is by the scattering coefficient vector σ that optimizes 2Upgrade the scattering center parameter sets
Figure BDA00002308719300127
Be parameter
Figure BDA00002308719300128
Valuation set.
Step 8 is according to described parameter sets
Figure BDA00002308719300129
Make up the super-resolution dictionary
Figure BDA000023087193001210
8a) determine dictionary
Figure BDA000023087193001211
Apart from the discrete value of dimension coordinate parameter x: with parameter sets
Figure BDA000023087193001212
In apart from centered by the dimension coordinate parameter x, length is ρ rNeighborhood in value, the interval of adjacent parameter x is made as ρ r/ N s, obtain dictionary
Figure BDA00002308719300131
The discrete value apart from the dimension coordinate parameter x, N wherein sBe super-resolution multiple, General N s=2,4,8 ...;
8b) determine dictionary
Figure BDA00002308719300132
The discrete value of azimuth dimension coordinate parameters y:
With parameter sets
Figure BDA00002308719300133
In azimuth dimension coordinate parameters y centered by, length is ρ aNeighborhood in value, the interval of adjacent parameter y is made as ρ a/ N s, obtain dictionary
Figure BDA00002308719300134
The discrete value of azimuth dimension coordinate parameters y;
8c) determine dictionary
Figure BDA00002308719300135
The discrete value of scattering center length parameter L:
With parameter sets In scattering center length parameter L centered by, length is ρ aNeighborhood in value, the interval of adjacent parameter L is made as ρ a/ N s, obtain dictionary
Figure BDA00002308719300137
The discrete value of scattering center length parameter L;
8d) determine dictionary
Figure BDA00002308719300138
Distributed scattering center position angle parameter
Figure BDA00002308719300139
Discrete value:
With parameter sets
Figure BDA000023087193001310
In distributed scattering center position angle parameter
Figure BDA000023087193001311
Be dictionary
Figure BDA000023087193001312
Distributed scattering center position angle parameter
Figure BDA000023087193001313
8e) according to above-mentioned steps determine apart from the dimension coordinate parameter x, azimuth dimension coordinate parameters y, scattering center length parameter L, distributed scattering center position angle parameter
Figure BDA000023087193001314
Discrete value is by formula<13〉produce the former subvector corresponding with the dictionary parameter combinations of discretize, and atom is carried out energy normalized, make up the super-resolution dictionary
Figure BDA000023087193001315
For:
D 2 ( x , y , L | &theta; ^ 2 ) = [ d ^ 1 , . . . , d ^ i , . . . , d ^ N 2 ] - - - < 28 >
Wherein, i represents atom sequence number, i=1...N 2, N 2Expression super-resolution dictionary
Figure BDA000023087193001317
The atom number.
Step 9 utilizes orthogonal matching pursuit OMP method to find the solution suc as formula<29〉0 norm optimization problem:
&sigma; 3 = arg min &sigma; | | &sigma; | | 0 , s . t . | | s - D 2 ( x , y , L | &theta; ^ 2 ) &CenterDot; &sigma; | | 2 &le; &epsiv; - - - < 29 >
σ wherein 3Be the scattering coefficient vector of optimizing, its solution procedure is as follows:
9a) input dictionary
Figure BDA000023087193001320
9b) initialization is about to signal margin r and is initialized as frequency domain observation signal matrix column vector s, and scattering coefficient vector σ is initialized as 0, and atom index vector a is initialized as sky, establishes primary iteration number of times k=1, and the beginning iteration;
9c) the related coefficient of Dictionary of Computing and signal margin r vector C
C = D 2 ( x , y , L | &theta; ^ 2 ) H &CenterDot; r - - - < 30 >
Wherein () HThe expression conjugate transpose, the sequence number of greatest member is a among the related coefficient vector C k, obtain atom index vector a and be:
a=[a 1,…,a k] <31>
9d) utilize least square method calculation method for scattering coefficient vector σ
Figure BDA00002308719300142
Wherein
Figure BDA00002308719300143
The expression pseudoinverse, D 2(:, a) be dictionary D 2Middle row number are a iThe matrix i=1 that consists of of k column vector ..., k, k are the current iteration number of times;
Upgrade surplus r:
r=s-D 2(:,a)·σ(a) <33>
Wherein σ (a) is a for sequence number among the scattering coefficient vector σ iThe column vector i=1 that consists of of k element ..., k;
9e) calculate reconstruct energy Ratios η k:
&eta; k = &Sigma; | | s k | | 2 2 &Sigma; | | s | | 2 2 - - - < 34 >
s k=D 2(:,a)·σ(a)
S wherein kBe reconstruction signal,
Figure BDA00002308719300145
Represent 2 norms square;
If 9f) η kK-1≤ δ stops iteration, and σ 3=σ wherein δ is the thresholding of the difference of adjacent iteration energy Ratios, gets δ=0.001; Otherwise k=k+1 also goes to step 9c).
Step 10 is by the scattering coefficient vector σ that optimizes 3Upgrade the scattering center parameter sets
Figure BDA00002308719300146
The super-resolution that obtains (x, y, L) is estimated set
Figure BDA00002308719300147
According to the scattering center parameter sets
Figure BDA00002308719300148
Estimating target and vitals geometries characteristic thereof.
For example, when radar image data for open MSTAR measured data in the position angle be that 80.774185 ° of angles of pitch are when being 15 ° T72 tank data, according to scattering center and the parameter sets thereof of final extraction
Figure BDA00002308719300151
The physical dimension of estimating the T72 tank is: T72 tank gun tube length degree is 6.4 meters, and the tank body length is 6.8 meters, and the total length of T72 tank is 9.4 meters, and the width valuation of T72 tank is 3.8 meters.
Effect of the present invention further specifies by following experiment to measured data:
1) experiment scene:
Synthetic-aperture radar SAR data and the position angle of testing used measured data and be disclosed MSTAR data centralization position angle and be 80.774185 ° of angles of pitch and be 15 ° T72 tank are that 0.307442 ° of angle of pitch is the SAR data of 17 ° D7 forklift, the centre frequency f of radar c=9.6GHz, bandwidth B=591MHz.T72 tank true geometric is of a size of: the long 6.41m of car body, overall width 3.52m, the long 6.155m of gun barrel, big gun be gun barrel extension elongation 3.035m forward the time.D7 forklift true geometric is of a size of: overall width 2.56m, vehicle commander 4.2m, overall height 3.294m, track shoe width 0.56m, track gage 1.981m, ground connection track length 2.72m.2) experiment content:
Be that 80.774185 ° of angles of pitch are 15 ° T72 tank MSTAR data for the position angle 2a), utilize coordinate samsara descent method to make up the super-resolution dictionary, obtain the set of scattering center parameter estimation by finding the solution 0 norm optimization problem.Fig. 4 is original T72 tank SAR image, according to the T72 tank image of the scattering center of extracting and parameter reconstruct thereof as shown in Figure 5, and by Fig. 4 and Fig. 5 accurate reconstruct target image of the present invention as can be known.
Be that 0.307442 ° of angle of pitch is 17 ° D7 forklift MSTAR data for the position angle 2b), utilize coordinate samsara descent method to make up the super-resolution dictionary, obtain the set of scattering center parameter estimation by finding the solution 0 norm optimization problem.Fig. 6 is original D7 forklift SAR image, according to the T72 tank image of the scattering center of extracting and parameter reconstruct thereof as shown in Figure 7, and by Fig. 6 and Fig. 7 accurate reconstruct target image of the present invention as can be known.
3) interpretation:
Table 1 the inventive method is processed T72 tank data convergence process
Step 3 Step 6 Step 9
The reconstruct energy Ratios 79.8% 83.7% 86.5%
Dictionary atom number 9030 63000 47000
The scattering center number 126 94 92
Table 2 the inventive method is processed D7 forklift data convergence process
Step 3 Step 6 Step 9
The reconstruct energy Ratios 84% 86.7% 88.7%
Dictionary atom number 4800 31125 29925
The scattering center number 83 57 57
Table 1 and table 2 have provided respectively the convergence situation that method of the present invention is processed reconstruct energy Ratios, dictionary atom number and scattering center number in T72 tank and the D7 forklift data procedures.Because step 3 supposition
Figure BDA00002308719300161
And only parameter (x, y, L) is carried out according to a preliminary estimate, so the reconstruct energy of step 3 is lower; When step 6 is considered distributed scattering center position angle on the basis of step 3
Figure BDA00002308719300162
The time, the reconstruct energy Ratios is improved, and the scattering center number of extraction reduces; The parameter resolution of dictionary increases in the step 9, and the reconstruct energy Ratios is improved, and the scattering center number also further reduces, and dictionary atom number is reduced, this be since step 3 to having utilized coordinate samsara decline technology between the step 9.The data convergence process shows that the inventive method can effectively extract scattering center in table 1, the table 2.
The physical dimension that can estimate T72 tank and D7 forklift according to scattering center and the parameter thereof of final extraction.
Table 3 is used for estimating the scattering center parameter of T72 tank gun tube length degree
Figure BDA00002308719300163
Table 3 shows, estimates that according to coordinate and the scattering center length of scattering center tank gun tube length degree is 6.4 meters.
Table 4 is used for estimating the scattering center parameter of T72 tank body length
Table 4 shows, estimates that according to coordinate parameters and the scattering center length of scattering center the tank body length is 6.8 meters.
The total length valuation that can be obtained the T72 tank by the object support district is 9.4 meters; Be half of T72 tank width according to the scattering center of T72 tank coboundary to the distance of gun barrel scattering center, the width valuation that obtains the T72 tank is 3.8 meters.
Table 5 is used for estimating the scattering center parameter of D7 forklift blade length
Figure BDA00002308719300171
Table 5 shows, estimates that according to coordinate parameters and the scattering center length of scattering center D7 forklift perching knife length is 3 meters.
Table 6 is used for estimating the scattering center parameter of D7 forklift width
Figure BDA00002308719300172
Table 6 shows, estimates that according to coordinate parameters and the scattering center length of scattering center D7 forklift width is 2.6 meters.
Table 7 is used for estimating the scattering center parameter of D7 forklift crawler width
Figure BDA00002308719300173
Table 7 shows, estimates that according to coordinate parameters and the scattering center length of scattering center D7 forklift crawler width is 0.6 meter.
Can estimate that by the crawler belt scattering center of extracting the ground connection track length of D7 forklift is 2.6 meters; Obtaining D7 forklift vehicle commander valuation by the object support district is 4.31 meters.
True geometric size in conjunction with T72 tank and D7 forklift, the physical dimension error of the target of the inventive method estimation and vitals thereof is in 6% as can be known, and experimental result explanation the inventive method can accurately be extracted the physical dimension of objective attribute target attribute scattering center feature and accurate estimating target and vitals thereof effectively.

Claims (4)

1. the radar target attribute scattering center feature extracting method based on Its Sparse Decomposition comprises the steps:
1) sets scattering center strength threshold ξ according to noise in the radar image, intensity in the radar image is defined as the strong scattering center greater than the scattering center of ξ, according to the strong scattering centre coordinate (x that detects, y) determine coordinate parameters x, the span of y, determine scattering center length L span by prior imformation, set distributed scattering center position angle Final definite scattering center parameter
Figure FDA00002308719200012
Set
Figure FDA00002308719200013
2) according to described parameter sets Make up dictionary
Figure FDA00002308719200015
2a) with dictionary
Figure FDA00002308719200016
Parameter sets
Figure FDA00002308719200017
Discretize, the interval that is about to the adjacent coordinates parameter x is made as a Range resolution element length ρ r, the interval of adjacent coordinates parameter y is made as an azimuth discrimination element length ρ a, the interval of adjacent scattering center length parameter L is made as ρ a
2b) according to the attribute scattering center model, produce the atom d of corresponding different parameters i(f, φ)
d i ( f , &phi; ) = exp ( - j 4 &pi;f c ( x i cos &phi; + y i sin &phi; ) ) &CenterDot;
sin c ( 2 &pi;f c L i sin ( &phi; - &phi; i &OverBar; ) ) - - - < 1 >
i=1,...N 0
Wherein i represents atom sequence number, N 0Expression is dictionary when (x, y, L) according to a preliminary estimate
Figure FDA000023087192000110
The atom number, exp () is natural exponential function, sinc () is Sinc function,
Figure FDA000023087192000111
Be set I group parameter after the discretize, f is the radar emission signal frequency, and φ is the radar beam position angle, and c is the light velocity;
To not homoatomic d i(f, φ) column vector, and former subvector carried out energy normalized, make up dictionary
Figure FDA000023087192000113
For:
D 0 ( x , y , L | &theta; ^ 0 ) = [ d ^ 1 , . . . , d ^ i , . . . , d ^ N 0 ]
d ^ i = vec ( d i ( f , &phi; ) ) | | vec ( d i ( f , &phi; ) ) | | 2 - - - < 2 >
Wherein vec () expression column vector operation, || || 2Be 2 norm operators;
3) utilize orthogonal matching pursuit OMP method to find the solution suc as formula<3〉0 norm optimization problem, by σ 1Upgrade the scattering center parameter sets
Figure FDA00002308719200021
Figure FDA00002308719200022
According to a preliminary estimate set for scattering center parameter (x, y, L);
&sigma; 1 = arg min &sigma; | | &sigma; | | 0 , s . t . | | s - D 0 ( x , y , L | &theta; ^ 0 ) &CenterDot; &sigma; | | 2 &le; &epsiv; - - - < 3 >
Wherein, σ is scattering coefficient vector to be optimized, σ 1Be the scattering coefficient vector of optimizing, s is the vectorization of frequency domain observation signal matrix column, || || 0Be 0 norm operator, ε is the energy error constraint factor, and the energy Ratios that accounts for the view picture radar image according to the object support district is determined;
4) according to described parameter sets
Figure FDA00002308719200025
Make up dictionary
4a) determine scattering center length L span according to prior imformation, the interval of adjacent scattering center length parameter L is made as ρ a, obtain dictionary
Figure FDA00002308719200027
The discrete value of scattering center length parameter L; Determine distributed scattering center position angle according to the orientation angular domain of radar return data recording
Figure FDA00002308719200028
Span is with adjacent distributions formula scattering center position angle parameter
Figure FDA00002308719200029
The interval be made as Obtain dictionary Distributed scattering center position angle parameter
Figure FDA000023087192000212
Discrete value; The scattering center coordinate parameters
Figure FDA000023087192000213
4b) according to scattering center length parameter L and the distributed scattering center position angle of discretize
Figure FDA000023087192000214
By formula<1〉produce former subvector, and atom is carried out energy normalized, make up dictionary
Figure FDA000023087192000215
For:
D 1 ( L , &phi; &OverBar; | &theta; ^ 1 ) = [ d ^ 1 , . . . , d ^ i , . . . , d ^ N 1 ] - - - < 4 >
N wherein 1The expression estimated parameter
Figure FDA000023087192000217
The time dictionary
Figure FDA000023087192000218
The atom number;
5) utilize orthogonal matching pursuit OMP method to find the solution suc as formula<5〉0 norm optimization problem, by σ 2Upgrade the scattering center parameter sets
Figure FDA000023087192000219
Figure FDA000023087192000220
Be parameter
Figure FDA000023087192000221
Valuation set;
&sigma; 2 = arg min &sigma; | | &sigma; | | 0 , s . t . | | s - D 1 ( L , &phi; &OverBar; | &theta; ^ 1 ) &CenterDot; &sigma; | | 2 &le; &epsiv; - - - < 5 >
σ wherein 2Be the scattering coefficient vector of optimizing;
6) according to described parameter sets
Figure FDA000023087192000224
Make up the super-resolution dictionary
Figure FDA000023087192000225
6a) with
Figure FDA000023087192000226
In coordinate parameters x centered by, length is ρ rNeighborhood in value, the interval of adjacent parameter x is made as ρ r/ N s, obtain dictionary
Figure FDA00002308719200031
The discrete value of coordinate parameters x, N sBe super-resolution multiple, General N s=2,4,8 ...; With
Figure FDA00002308719200032
In y centered by, length is ρ aNeighborhood in value, the interval of adjacent parameter y is made as ρ a/ N s, obtain dictionary
Figure FDA00002308719200033
The discrete value of coordinate parameters y; With
Figure FDA00002308719200034
In L centered by, length is ρ aNeighborhood in value, the interval of adjacent parameter L is made as ρ a/ N s, obtain dictionary
Figure FDA00002308719200035
The discrete value of scattering center length parameter L; Distributed scattering center position angle parameter
Figure FDA00002308719200036
6b) according to the dictionary parameter x of discretize, y, L is by formula<1〉produce former subvector, and atom is carried out energy normalized, make up the super-resolution dictionary
Figure FDA00002308719200037
D 2 ( x , y , L | &theta; ^ 2 ) = [ d ^ 1 , . . . , d ^ i , . . . , d ^ N 2 ] - - - < 6 >
Wherein, N 2Expression super-resolution dictionary The atom number;
7) utilize orthogonal matching pursuit OMP method to find the solution suc as formula<7〉0 norm optimization problem, by σ 3Upgrade the scattering center parameter sets
Figure FDA000023087192000310
The super-resolution that obtains (x, y, L) is estimated set
Figure FDA000023087192000311
With target and vitals geometries characteristic thereof;
&sigma; 3 = arg min &sigma; | | &sigma; | | 0 , s . t . | | s - D 2 ( x , y , L | &theta; ^ 2 ) &CenterDot; &sigma; | | 2 &le; &epsiv; - - - < 7 >
σ wherein 3Be the scattering coefficient vector of optimizing.
2. method according to claim 1, wherein the described orthogonal matching pursuit OMP method of utilizing of step 3 is found the solution suc as formula<3〉0 norm optimization problem, carry out as follows:
3a) input dictionary
Figure FDA000023087192000314
3b) initialization is about to signal margin r and is initialized as frequency domain observation signal matrix column vector s, and scattering coefficient vector σ is initialized as 0, and atom index vector a is initialized as sky, establishes primary iteration number of times k=1, and the beginning iteration;
3c) the related coefficient of Dictionary of Computing and signal margin r vector C
C = D 0 ( x , y , L | &theta; ^ 0 ) H &CenterDot; r - - - < 8 >
Wherein () HThe expression conjugate transpose, the sequence number of greatest member is a among the related coefficient vector C k, can get atom index vector a and be:
a=[a 1,...,a k] <9>
3d) utilize least square method calculation method for scattering coefficient vector σ
Wherein The expression pseudoinverse, D 0(:, a) be dictionary D 0Middle row number are a iThe matrix i=1 that consists of of k column vector ..., k, k are the current iteration number of times;
Upgrade surplus r:
r=s-D 0(:,a)·σ(a) <11>
Wherein σ (a) is a for sequence number among the scattering coefficient vector σ iThe column vector i=1 that consists of of k element ..., k;
3e) calculate reconstruct energy Ratios η k
&eta; k = &Sigma; | | s k | | 2 2 &Sigma; | | s | | 2 2 - - - < 12 >
s k=D 0(:,a)·σ(a)
S wherein kBe reconstruction signal,
Figure FDA00002308719200044
Represent 2 norms square;
If 3f) η kK-1≤ δ stops iteration, and wherein δ is the thresholding of the difference of adjacent iteration energy Ratios, gets δ=0.001; Otherwise k=k+1 also goes to step 3c).
3. method according to claim 1, wherein the described orthogonal matching pursuit OMP method of utilizing of step 5 is found the solution suc as formula<5〉0 norm optimization problem, carry out as follows:
5a) input dictionary
Figure FDA00002308719200045
5b) initialization is about to signal margin r and is initialized as frequency domain observation signal matrix column vector s, and scattering coefficient vector σ is initialized as 0, and atom index vector a is initialized as sky, establishes primary iteration number of times k=1, and the beginning iteration;
5c) the related coefficient of Dictionary of Computing and signal margin r vector C
C = D 1 ( L , &phi; &OverBar; | &theta; ^ 1 ) H &CenterDot; r - - - < 13 >
Wherein () HThe expression conjugate transpose, the sequence number of greatest member is a among the related coefficient vector C k, can get atom index vector a and be:
a=[a 1,...,a k] <14>
5d) utilize least square method calculation method for scattering coefficient vector σ
Figure FDA00002308719200051
Wherein
Figure FDA00002308719200052
The expression pseudoinverse, D 1(:, a) be dictionary D 1Middle row number are a iThe matrix i=1 that consists of of k column vector ..., k, k are the current iteration number of times;
Upgrade surplus r:
r=s-D 1(:,a)·σ(a) <16>
Wherein σ (a) is a for sequence number among the scattering coefficient vector σ iThe column vector i=1 that consists of of k element ..., k;
5e) calculate reconstruct energy Ratios η k
&eta; k = &Sigma; | | s k | | 2 2 &Sigma; | | s | | 2 2 - - - < 17 >
s k=D 1(:,a)·σ(a)
S wherein kBe reconstruction signal,
Figure FDA00002308719200054
Represent 2 norms square;
If 5f) η kK-1≤ δ stops iteration, and wherein δ is the thresholding of the difference of adjacent iteration energy Ratios, gets δ=0.001; Otherwise k=k+1 also goes to step 5c).
4. method according to claim 1, wherein the described orthogonal matching pursuit OMP method of utilizing of step 7 is found the solution suc as formula<7〉0 norm optimization problem, carry out as follows:
7a) input dictionary
Figure FDA00002308719200055
7b) initialization is about to signal margin r and is initialized as frequency domain observation signal matrix column vector s, and scattering coefficient vector σ is initialized as 0, and atom index vector a is initialized as sky, establishes primary iteration number of times k=1, and the beginning iteration;
7c) the related coefficient of Dictionary of Computing and signal margin r vector C
C = D 2 ( x , y , L | &theta; ^ 2 ) H &CenterDot; r - - - < 18 >
Wherein () HThe expression conjugate transpose, the sequence number of greatest member is a among the related coefficient vector C k, obtain atom index vector a and be:
a=[a 1,...,a k] <19>
7d) utilize least square method calculation method for scattering coefficient vector σ
Figure FDA00002308719200061
Wherein
Figure FDA00002308719200062
The expression pseudoinverse, D 2(:, a) be dictionary D 2Middle row number are a iThe matrix i=1 that consists of of k column vector ..., k, k are the current iteration number of times;
Upgrade surplus r:
r=s-D 2(:,a)·σ(a) <21>
Wherein σ (a) is a for sequence number among the scattering coefficient vector σ iThe column vector i=1 that consists of of k element ..., k;
7e) calculate reconstruct energy Ratios η k:
&eta; k = &Sigma; | | s k | | 2 2 &Sigma; | | s | | 2 2 - - - < 22 >
s k=D 2(:,a)·σ(a)
S wherein kBe reconstruction signal,
Figure FDA00002308719200064
Represent 2 norms square;
If 7f) η kK-1≤ δ stops iteration, and wherein δ is the thresholding of the difference of adjacent iteration energy Ratios, gets δ=0.001; Otherwise k=k+1 also goes to step 7c).
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